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Titlebook: Water Waves and Ship Hydrodynamics; An Introduction R. Timman,A. J. Hermans,G. C. Hsiao Book 1985 Springer Science+Business Media B.V. 1985

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11#
發(fā)表于 2025-3-23 11:40:04 | 只看該作者
Linear Theory of Water Waves, and the equation of continuity for a non-viscous incompressible fluid moving under gravity. Throughout the book, in most considerations the motion is assumed to be irrotational and hence the existence of a velocity potential function is ensured in simply connected regions. In this case the equation
12#
發(fā)表于 2025-3-23 15:04:07 | 只看該作者
13#
發(fā)表于 2025-3-23 18:31:42 | 只看該作者
14#
發(fā)表于 2025-3-23 23:20:54 | 只看該作者
15#
發(fā)表于 2025-3-24 03:25:40 | 只看該作者
Irregular and Non-Linear Waves,ace and time. Section 3.1 contains a brief description of the Wiener spectrum in connection with generalized Fourier representations for the surface waves [2], [13]. In this way we see how one may represent the surface wave by a superposition of harmonic waves with amplitudes being a stochastic proc
16#
發(fā)表于 2025-3-24 08:19:23 | 只看該作者
17#
發(fā)表于 2025-3-24 11:09:59 | 只看該作者
Book 1985ese notes grew. Those of us privi- leged to be present during that time will never forget the experience. Rein Tirnrnan is not easily forgotten. His seemingly inexhaustible energy completely overwhelmed us. Who could forget the numbing effect of a succession of long wine filled evenings of lively co
18#
發(fā)表于 2025-3-24 15:12:21 | 只看該作者
19#
發(fā)表于 2025-3-24 21:28:46 | 只看該作者
Linear Theory of Water Waves, assumed to be irrotational and hence the existence of a velocity potential function is ensured in simply connected regions. In this case the equation of continuity for the velocity of fluid is then reduced to the familiar Laplace equation for the velocity potential function.
20#
發(fā)表于 2025-3-25 00:35:03 | 只看該作者
Linear Theory of Water Waves, assumed to be irrotational and hence the existence of a velocity potential function is ensured in simply connected regions. In this case the equation of continuity for the velocity of fluid is then reduced to the familiar Laplace equation for the velocity potential function.
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